Matches in SemOpenAlex for { <https://semopenalex.org/work/W72483091> ?p ?o ?g. }
- W72483091 endingPage "435" @default.
- W72483091 startingPage "391" @default.
- W72483091 abstract "In summary, extensive studies of the dispersive quasiparticle states in optimally doped untwinned single crystals of Y123 using polarization-dependent angle-resolved photoelectron spectroscopy have illuminated a number of points regarding the electronic structure of this material. Based on analysis of the Ba 5p core level and inference from other surface-sensitive probes, the observed surface-to-bulk intensity ratio can be reproduced with a simple model incorporating a mixed surface termination of BaO and CuO3 regions. Furthermore, with an electron attenuation length in this material of approximately 5 , the bulk of the photoemission intensity arises from the surface and first subsurface CuO2 planes, with significant attenuation of the signal from the bulk chains. Extensive arguments, based on photon polarization dependence, photon energy dependence, intensity variations between twinned, untwinned, and Y124 crystals, and oxygen, Co, and Pr doping results, favor attribution of the intense, narrow feature found near the Y point to a surface-related chain state. This feature, which appears at both X and Y in twinned crystals, is extrinsic to the bulk electronic states of Y123, and contaminates data in the crucial near-EF region in crystals which are not exceptionally well detwinned. The measured band dispersions clearly reveal two plane-derived quasiparticle states, one with a binding energy of 0.22 eV at Γ, and the other with 0.53 eV, which are associated with the antibonding and bonding bilayer bands. The former disperses upward to form a van Hove singularity with a binding energy of 0.13 eV at X, while the latter is weakly dispersive along ΓX, and disperses rapidly upward along XS. While no measurable c-axis dispersion is seen in the antibonding band by changing the photon energy, the bonding band shifts upward by 0.11 eV when hv is changed from 28eV to 21eV. Observation of two distinct plane states and c-axis dispersion provides clear evidence for bilayer splitting in Y123, consistent with the simplest band-theoretical arguments. Quantitative Fermi surface determination based on a momentum-space DOS analysis reveals a strongly nested inner Fermi surface pocket centered on S attributed to the CuO2 bonding pdσ bands. The bilayer splitting of the plane bands, which is clearly resolved in polarization-dependent energy-distribution curves appears as a more weakly resolved outer sheet in the k-space data. Vestiges of the principal chain sheet are also weakly apparent in some of the data, but are significantly suppressed, consistent with a strongly modified surface chain termination. The data show no sign of a “stick” Fermi surface centered at S, consistent with previous measurements but disagreeing with LMTO calculations. Evidence for antiferromagnetic shadow Fermi surfaces appears to be lacking in optimally doped Y123, supporting a structural origin for such features seen in Bi2212. Finally, the presence of leading-edge shifts with a k-dependence characteristic of pure d-wave order parameter untwinned Y123 has been observed. These shifts cannot be conclusively associated with the onset of the superconducting transition due to the surface instability of this material above Tc, but are consistent with a highly anisotropic superconducting gap of d-wave form. The lack of phase information makes it difficult to exclude the possibility of symmetries such as d + id or highly anisotropic s-wave mimicking the d-wave form." @default.
- W72483091 created "2016-06-24" @default.
- W72483091 creator A5018124544 @default.
- W72483091 creator A5025712547 @default.
- W72483091 date "2001-01-01" @default.
- W72483091 modified "2023-09-27" @default.
- W72483091 title "Chapter 201 Angle-resolved photoemission studies of untwinned yttrium barium copper oxide" @default.
- W72483091 cites W1000096099 @default.
- W72483091 cites W135067810 @default.
- W72483091 cites W1482731350 @default.
- W72483091 cites W1485300768 @default.
- W72483091 cites W1517354136 @default.
- W72483091 cites W1520939936 @default.
- W72483091 cites W1522870691 @default.
- W72483091 cites W1529423760 @default.
- W72483091 cites W1550484900 @default.
- W72483091 cites W1617352475 @default.
- W72483091 cites W1624028143 @default.
- W72483091 cites W1628526237 @default.
- W72483091 cites W1660624961 @default.
- W72483091 cites W1672911329 @default.
- W72483091 cites W1677951991 @default.
- W72483091 cites W1964181044 @default.
- W72483091 cites W1964394185 @default.
- W72483091 cites W1965959302 @default.
- W72483091 cites W1966138251 @default.
- W72483091 cites W1968624895 @default.
- W72483091 cites W1972270507 @default.
- W72483091 cites W1973663126 @default.
- W72483091 cites W1974944803 @default.
- W72483091 cites W1977008309 @default.
- W72483091 cites W1978799946 @default.
- W72483091 cites W1980233950 @default.
- W72483091 cites W1980660637 @default.
- W72483091 cites W1981937780 @default.
- W72483091 cites W1982867359 @default.
- W72483091 cites W1985118247 @default.
- W72483091 cites W1985395992 @default.
- W72483091 cites W1986856835 @default.
- W72483091 cites W1987485828 @default.
- W72483091 cites W1987598609 @default.
- W72483091 cites W1988371505 @default.
- W72483091 cites W1989482936 @default.
- W72483091 cites W1993976706 @default.
- W72483091 cites W1994350882 @default.
- W72483091 cites W1994529426 @default.
- W72483091 cites W1995840085 @default.
- W72483091 cites W1996634745 @default.
- W72483091 cites W1998154630 @default.
- W72483091 cites W2003632850 @default.
- W72483091 cites W2006706015 @default.
- W72483091 cites W2008739268 @default.
- W72483091 cites W2008946274 @default.
- W72483091 cites W2009101057 @default.
- W72483091 cites W2009888181 @default.
- W72483091 cites W2010972043 @default.
- W72483091 cites W2013857926 @default.
- W72483091 cites W2014437371 @default.
- W72483091 cites W2017463185 @default.
- W72483091 cites W2018314213 @default.
- W72483091 cites W2019023044 @default.
- W72483091 cites W2030898162 @default.
- W72483091 cites W2031982124 @default.
- W72483091 cites W2032551484 @default.
- W72483091 cites W2033433860 @default.
- W72483091 cites W2036641967 @default.
- W72483091 cites W2037481961 @default.
- W72483091 cites W2039081246 @default.
- W72483091 cites W2040013347 @default.
- W72483091 cites W2041911208 @default.
- W72483091 cites W2043688643 @default.
- W72483091 cites W2045897140 @default.
- W72483091 cites W2046013658 @default.
- W72483091 cites W2046021903 @default.
- W72483091 cites W2048014609 @default.
- W72483091 cites W2048531892 @default.
- W72483091 cites W2050182395 @default.
- W72483091 cites W2051651396 @default.
- W72483091 cites W2055891591 @default.
- W72483091 cites W2056200009 @default.
- W72483091 cites W2061099829 @default.
- W72483091 cites W2062106088 @default.
- W72483091 cites W2064042410 @default.
- W72483091 cites W2065141250 @default.
- W72483091 cites W2065399159 @default.
- W72483091 cites W2066440625 @default.
- W72483091 cites W2066764094 @default.
- W72483091 cites W2067405508 @default.
- W72483091 cites W2069699601 @default.
- W72483091 cites W2069700924 @default.
- W72483091 cites W2070548001 @default.
- W72483091 cites W2073379794 @default.
- W72483091 cites W2076308919 @default.
- W72483091 cites W2078576314 @default.
- W72483091 cites W2079308174 @default.
- W72483091 cites W2079471413 @default.
- W72483091 cites W2082040708 @default.
- W72483091 cites W2084935150 @default.